Method and apparatus for cell analysis

ABSTRACT

A method and apparatus for investigating the electroporation properties of cells suspended in a fluid. The apparatus comprises: first and second substrates spaced apart from each other; a first array of electrodes formed on a surface of the first substrate; at least one electrode formed on the surface of the second substrate facing the first array of electrodes. The at least one electrode and the first array of electrodes thereby define the upper and lower bounds of an analysis volume for receiving the fluid, the analysis volume comprising an array of volume portions. Circuitry is arranged to modify the amplitude and duration of a voltage applied to at least the first array of electrodes so as to generate and modify an electric field in one or more volume portions of the device. Thus, the 10 electroporation properties of the cells may be investigated by generating electric fields of different amplitudes or durations in one or more volume portions of the apparatus with the fluid placed therein.

FIELD OF THE INVENTION

This invention relates to a method and apparatus for analysing cells, and more particularly to analysing cells suspended in a fluid.

BACKGROUND OF THE INVENTION

Cell analysis can be performed in different ways. Known techniques for cell analysis include optical inspection of a sample containing the cells (e.g. placing a drop of blood between two microscope glass plates), mechanical deformation of the cell, and laser-based cell counting (otherwise known as flow cytometry). Though often very precise, these methods are limited in scope and versatility.

Undertaking cell analysis to investigate parameters of cells is important in relation to a cell manipulation technique called Electroporation. Electroporation is a technique that uses an electric field to create pores in a cell membrane so that molecules (such as drugs or genes) can be transferred into the cell.

Electroporation is important in the context of gene therapy because controlled transport of DNA into a cell is required. Although viral vectors are known to be a very efficient way of undertaking gene delivery to a cell, the use of the viral vectors is not risk free (D. J. Wells, Gene therapy 11, pp 1363, 2004). Non-viral alternatives such as electroporation are therefore of particular interest because they may avoid the need for additional chemicals or materials to open the cell membranes. Electroporation also has the advantage that it may reduce the possibility of cell contamination.

In devices that are typically used for electroporation, multiple cells in a suspension fluid are electroporated at once. Examples of such devices are the electroporation generators of BTX Molecular Delivery Systems, or the Cloning Gun™ Electroporation System of Tritech Research. These devices, however, are not ideal because the electric field varies within the device arrangement. As a consequence of this drawback, typically 90% of the cells do not survive the electroporation process.

Currently, the mechanism of electroporation is not very well understood. It is however known that selecting an appropriate electric waveform can optimise the process (Huang en Rubinski, Sensors and Actuators A 89, pp 242, 2001). Such optimal electroporation parameters are dependent upon the cell type. Thus, the optimisation of the electroporation parameters has to be performed for every single cell type.

Using known cell analysis techniques, including those mentioned above, the analysis and optimisation of cell properties is a labour intensive and time consuming process. It is therefore desirable to create an improved cell analysis technique for the controlled inspection and/or analysis of cells such that the electroporation properties of the cells may be investigated. It is also desirable to enable such analysis to be undertaken using a single device and/or procedure.

SUMMARY OF THE INVENTION

According to an aspect of the invention, there is provided a cell analysis device for investigating the electroporation properties of cells suspended in a fluid, the device comprising:

first and second substrates spaced apart from each other;

a first array of electrodes formed on a surface of the first substrate;

at least one electrode formed on the surface of the second substrate facing the first array of electrodes, the at least one electrode and the first array of electrodes thereby defining the upper and lower bounds of an analysis volume for receiving the fluid, the analysis volume comprising an array of volume portions; and

circuitry arranged to modify the amplitude or duration of a voltage applied to at least the first array of electrodes so as to generate and modify an electric field in one or more volume portions of the device.

Thus, there is provided apparatus for analysing the electroporation properties of cells in which the applied electric field can be controlled on an individual cell basis. Further, the apparatus may be used to find optimal electroporation parameters for a plurality of cells using a single measurement procedure.

According to another aspect of the invention, there is provided a method of operating a cell analysis device to investigate the electroporation properties of cells suspended in a fluid, the device comprising two spaced apart substrates with an analysis volume defined therebetween and the analysis volume comprising an array of volume portions, and the method comprising the step of generating electric fields of different amplitudes or durations in one or more volume portions of the device with the fluid placed therein.

According to yet another aspect of the invention, there is provided a method of manufacturing a cell analysis device for investigating the electroporation properties of cells suspended in a fluid, the method comprising the steps of:

forming a first array of electrodes on a surface of a first substrate;

forming at least one electrode on the surface of a second substrate facing the first array of electrodes, spacing first and second substrates apart from each other with the surfaces facing each other, the at least one electrode and the first array of electrodes thereby defining the upper and lower bounds of an analysis volume for receiving the fluid, the analysis volume comprising an array of volume portions; and

providing circuitry to modify the amplitude or duration of a voltage applied to at least the first array of electrodes such that an electric field may be generated or modified in one or more volume portions of the device.

According to another aspect of the invention, there is provided a method of manufacturing a cell analysis device for investigating the electroporation properties of cells suspended in a fluid, the method comprising the steps of:

disassembling a liquid crystal display; and

removing the liquid crystal material.

The invention therefore provides for a reduction in the time and labour required to investigate the electroporation parameters of cells. Furthermore, the parameters may be used to improve the yield of an electroporation process.

The analysis device may be of an active matrix based design. Also the device may enable the cells to be electrically transported and trapped using the known physical phenomenon of dielectrophoresis (DEP), electrophoresis, electro-osmosis or electro-hydrodynamics.

BRIEF DESCRIPTION OF DRAWINGS

Examples of the invention will now be described in detail with reference to the accompanying drawings, in which:

FIG. 1 shows a matrix cell analysis device according to an embodiment of the invention;

FIG. 2 is a cross-sectional view along the line X-X of FIG. 1 that illustrates the device being used to analyse the electroporation properties of cells suspended in a fluid;

FIG. 3 shows a matrix cell analysis device according to an alternative embodiment of the invention;

FIG. 4 is a schematic circuit diagram of the device shown in FIG. 3;

FIG. 5 illustrates the operation of the device of FIG. 3 according to an embodiment of the invention;

FIG. 6 is a timing diagram of select pulses for the device operation illustrated in FIG. 5;

FIG. 7 illustrates a modification of the circuit diagram shown in FIG. 4; and

FIG. 8 illustrates the operation of the device of FIG. 3 according to another embodiment of the invention.

Like reference numeral refer to like elements throughout.

DETAILED DESCRIPTION OF THE INVENTION

Referring to FIG. 1, a matrix-based cell analysis device according to a first embodiment of the invention is shown. The cell analysis device comprises first 10 and second 12 substrates arranged parallel to and spaced apart from each other, wherein the first substrate 10 is positioned vertically below the second substrate 12.

A first array of electrodes 14 a-14 d (hereinafter referred to as the first electrode array 14) is provided on the upwardly facing surface of the first substrate 10. The electrodes 14 a-14 d of the first electrode array 14 are generally elongate and extend in the lateral direction (the lateral direction being indicated generally by the arrow labelled “L”) and are arranged such that they are substantially parallel to and spaced apart longitudinally from each other (the longitudinal direction being indicated generally by the arrow labelled “M”).

An example of a suitable material for the electrodes is indium tin oxide (ITO). Of course, any other suitable material may be used to form the electrodes, such as Pt, Au, Ti, Ta etc. Optionally, the electrodes could be covered by a thin dielectric layer in order to prevent corrosion of the electrode or the occurrence of electrolysis in water based fluids.

A second array of electrodes 16 a-16 f (hereinafter referred to as the second electrode array 16) is provided on the downwardly facing surface of the second substrate 12. In other words, the second electrode array 16 is formed on the surface of the second substrate 12 that faces the first substrate 10 and its first electrode array 14. The electrodes 16 a-16 f of the second electrode array 16 are generally elongate, extend in the longitudinal direction, and are arranged such that they are substantially parallel to and spaced apart laterally from each other.

Thus, the electrode arrays define an upper and lower bounds of a analysis volume 18 in which a fluid containing cells can be placed for analysis. The portion of the volume between a crossing of an electrode 14 a of the first electrode array 14 and an electrode 16 f of the second electrode array 16 defines a portion of the analysis volume (illustrated by shaded region labelled “P”).

The resultant matrix configuration (referred to as a “passive matrix” in the field of Liquid Crystal Display technology) therefore has a set of row electrodes at one side of the volume, and a set of column electrodes at the other side of the volume. In the embodiment shown in FIG. 1, the row electrodes are the electrodes of the first electrode array 14, and the column electrodes are the electrodes of the second electrode array 16.

A voltage driver circuit (not shown) is electrically connected to the first 14 and second 16 electrode arrays and adapted to modify the amplitude and duration of a voltage applied to the electrode arrays. Application of a voltage to both an electrode 14 a of the first electrode array 14 and an electrode 16 f of the second electrode array 16 generates an electric field in the volume portion P between the crossing of the electrodes. Thus, the electroporation properties of a cell suspended in a liquid and positioned within the volume portion P may be investigated by generating an electric field in the volume portion P. In other words, by positioning a cell in the volume portion P and applying a voltage to the electrodes that cross over to define the volume portion P, the cell can be electroporated. Once the electorporation is finished, the cell can be inspected or investigated as necessary. Such an investigation process may include the steps of optically inspecting the electroporated cell or measuring parameters of the cell such as its impedance.

Thus, by applying a voltage to a specific electrode in the first electrode array 14 and to an electrode in the second electrode array 16, an electric field can be generated in a particular portion of the analysis volume 18. The portion of the analysis volume 18 within which the electric field is generated will correspond to the crossing location of the electrodes to which a voltage is applied. It will therefore be appreciated that portions of the analysis volume 18 can be addressed by applying voltages to the first 14 and second 16 electrode arrays. Such an addressing process may be controlled by suitable control means in order to generate an electric field in one or more volume portions as may be required.

Voltages of differing amplitudes and/or durations may be applied to the electrodes of each array. In this way, electric fields of different magnitudes and duration can be generated in more than one volume portion at the same time. More than one cell can therefore be electroporated at once, wherein the electorporation parameters may differ between the cells.

A better understanding of this process may be obtained by referring to FIG. 2. FIG. 2 is a cross-sectional view along the line X-X of FIG. 1 and illustrates the analysis device being used to electroporate cells 20 suspended in a fluid 22.

The fluid 22 containing cells 20 for analysis is provided in the analysis volume 18. Preferably, at least one of the first 10 and second 12 substrates is formed with a fluidic system (not illustrated) for guiding the fluid 22 to a preferred location within the analysis volume 18. For example, such a fluidic system may be formed from at least one channel that is provided in the substrate along which the fluid 22 is guided to flow. Alternatively, the channels may be built up on the substrate using for example a photoresist layer such as SU-8. Further, the cells 20 within the fluid may be positioned between opposing electrodes using the known physical phenomenon of dielectrophoresis (DEP) electrophoresis, electro-osmosis or electro-hydrodynamics.

DEP is a physical phenomenon whereby neutral particles, when subject to non-uniform, time stationary (DC) to time varying (AC) electric fields, experience a net force directed towards locations with increasing (pDEP) or decreasing (dDEP) field intensity. The intensity of the dielectrophoretic force, in addition to its direction, strongly depends on the dielectric and conductive properties of the particles and on the medium in which the body is immersed. Of course, it should be understood that these properties may also vary as a function of frequency for AC electric fields. Further information about the theory of DEP can be found in a paper published by H. A. Pohl entitled “Dielectrophoresis” (Cambridge University Press, Cambridge, 1978), the contents of which are hereby incorporated by reference.

By applying a voltage to the electrode 16 d of the second electrode array at the same time that voltages of differing durations and/or magnitudes are applied to the first 14 a and second 14 b electrodes of the first electrode array 14, first 20 a and second 20 b cells positioned in first 24 and second 26 volume portions, respectively, are electroporated under different electric fields. Thus, a comparison between the results of the electroporation process for the first 20 a and second 20 b cell can be made. This concept can be extended to electroporate any number of cells suspended in a liquid, wherein each cell is positioned in a different volume portion and each volume portion is defined between the crossing of an electrode in the first electrode array 14 and an electrode in the second electrode array 16.

By varying the duration and/or the amplitude of the voltage applied to the electrodes of the electrode arrays, a plurality of cells can be electroporated under different electroporation parameters using a single electroporation procedure. In other words, the electroporation properties of multiple cells may be investigated by generating electric fields of different amplitudes or durations in one or more volume portions of the analysis device.

The basic structure of the device shown in FIG. 1 is composed of two substantially flat substrates which are separated by a thin gap in order to form a thin flat device. Although not essential to the invention, the thickness of such a separation may be defined by spacers (not shown) positioned between the first 10 and second 12 substrates. Furthermore, it is envisaged that the distance between the substrates would typically be in the range of 5 to 50 μm, and more preferably in the range of 10 to 30 μm. However, it should also be understood that the device may further comprise adjustment means for adjusting the spacing between the first 10 and second 12 substrates. In this way, the device may cater for differing sizes of cells.

The skilled reader will also appreciate that the device of FIG. 1 has a structure similar to that of a conventional passive matrix liquid crystal display (LCD), wherein the liquid crystal has been removed from between the substrates. It is therefore envisaged that known technology and techniques currently used to manufacture passive matrix LCDs may be used to manufacture a cell analysis device according to an embodiment of the invention.

Referring now to FIG. 3, a matrix cell analysis device according to an alternative embodiment of the invention is shown. The cell analysis device comprises first 30 and second 32 substrates parallel to and spaced apart from each other, the first substrate 30 being positioned vertically below the second substrate 32. Although not essential to the invention, the separation distance may be defined by spacers (not shown) positioned between the first 30 and second 32 substrates. Alternatively, the device may comprise adjustment means for adjusting the spacing between the first 30 and second 32 substrates. In this way, the device may cater for differing sizes of cells.

A first array of electrodes 34 (hereinafter referred to as the first electrode array) is provided on the upwardly facing surface of the first substrate 30. The electrodes 34 of the first electrode array are arranged to form a matrix comprising rows and columns of spaced apart electrodes 34. The electrodes 34 are conventional thin-film structures formed from ITO. Of course, any other suitable manufacturing techniques and material may be used to form the electrodes.

A single plate electrode 36 (hereinafter referred to as the common electrode 36) is provided on the downwardly facing surface of the second substrate 32. In other words, the common electrode 36 is formed on the surface of the second substrate 32 that faces the first electrode array. The common electrode 36 is a thin film structure formed from ITO and arranged such that it covers a substantial portion of the lower surface of the second substrate 32. In this way, the common electrode 36 is positioned vertically above the first electrode array such that it covers all of the electrodes 34 in the first electrode array.

Thus, the common electrode 36 and the first electrode array respectively define an upper and lower bounds of an analysis volume 38 in which a fluid containing cell can be placed for analysis. The portion of the analysis volume between the common electrode 36 and an electrode 34 of the first electrode array defines a first portion of the analysis volume (as illustrated by shaded region labelled “P”).

Although not essential to the invention, the second substrate 32 and the common electrode 36 are at least partially transparent. In this way, liquid provided in the analysis volume may be optically investigated using the naked eye or suitable optical equipment positioned externally to the device. Of course, the first substrate 30 and its respective electrodes 34 may instead be at least partially transparent in an alternative embodiment of the invention.

Voltage driving circuitry (not shown) is electrically connected to the first electrode array via row conductors 40, column conductors 42 and an array of switching elements 44. The row conductors 40, column conductors 42 and switching elements 44 are thin film structures and formed on the upper surface of the first substrate 30 in the spaces provided between the electrodes 34 of the first electrode array. Further, as mentioned in the previous paragraph, these thin film structures may be at least partially transparent to further simplify optical inspection of the analysis volume. Typically, the thin film structures may only cover a relatively small portion of the surface area and may be formed by non-transparent materials such as Al and amorphous Si etc.

Each electrode 34 of the first electrode array is electrically connected to a row conductor 40 and a column conductor 42 via a switching element 44. The resultant matrix configuration (commonly known as an “active matrix” in the field of Liquid Crystal Display technology) is fundamentally different from a simple passive matrix structure by the fact that, in an active matrix, the addressing scheme and the electric activation of each volume portion is decoupled. In other words, each volume portion is isolated from the rest of the analysis volume and connected to the addressing electronics solely via a switching element. Thus, each volume portion has its own switching element for regulating the electric field. Each volume portion can therefore be individually addressed during a short time and then substantially isolated from the remaining volume portions during the rest of the time frame.

Two main types of switching elements are commonly used in active matrices: diodes (e.g. Metal-Insulator-Metal (MIM) NIP, PIN and Shottky) and transistors (TFT: Thin Film Transistor). Thin film transistors (TFTs) are widely used as switching elements in LCDs due to their superior optical performance. However, diodes have the advantage of being relatively simple to fabricate. In the embodiment of FIG. 3, the switching elements are TFTs and the number of TFTs is the same as the number of volume portions provided by the device.

Referring to FIG. 4, each TFT 44 is connected electrically to a row conductor 40 and column conductor 42 of the device. More specifically, the TFTs 44 each have their source connected to a column conductor 42, their gate connected to a row conductor 40 and their drain connected to an electrode 44 of the first electrode array.

When a TFT 44 is addressed electrically by its respective row conductor 40 and column conductor 42, the selected electrode 34 in the device (i.e. an addressed volume portion) is charged up by the source-drain current of the TFT 44 as it is turned on. In other words, in the “on” state, a TFT 44 switching element provides a strongly non-linear response to an addressing signal, which allows fast charging (typically 2 to 10 μs) of a volume portion capacitor composed of an electrode 34 of the first electrode array and the common electrode 36 of the second substrate 32.

In the “off” state, the electric charge is held on the electrode 34, which becomes isolated from the rest of the device volume portions. This ensures a steady state for the electric field established in the volume portion.

A row scanner 46 (which may be otherwise referred to as a select scanner) is provided to sequence through rows of the TFT array by controlling the state (on or off) of TFTs along a row. Also, a column driver 48 (which may be otherwise referred to as a data scanner) is provided to sequence through columns and provide appropriate voltages to the TFTs. Preferably, the data is provided to all columns simultaneously in a so-called line-at-a-time addressing method.

When a row R_(i) is addressed, all the gates of the TFTs of that row are activated. When the columns C₁, C₂, C₃ etc are provided with an activation signal and all other columns are provided with a non-activation signal (such as the same voltage as is present on the common electrode), only the volume portions R_(i)C₁, R_(i)C₂, R_(i)C₃, etc. are activated (i.e. all electrodes in the row will receive a voltage from their column).

The device shown in FIG. 4 contains m columns and n rows. The row scanner 46 progressively scans the TFT array by turning on or off the TFTs in row 1, followed by row 2, and through to and ending with row n. When row 1 is selected, the column driver 48 applies different voltage levels to each column from column 1 to column m.

The selected row is then advanced and the new voltages are applied to the columns.

It will therefore be appreciated that each electrode 34 of the first electrode array (and therefore each volume portion) can be addressed individually, wherein the voltage applied to each electrode 34 may be controlled.

Of course, the column driver 48 may be arranged to apply a different predetermined voltage to each column, while the row scanner 46 is arranged to progressively scan the rows of the TFT array and turn on or off each row for differing amounts of time. In this way, the two axes of the TFT array are used to vary the duration and the amplitude of the voltage applied to different volume portion of the device.

This concept is illustrated in FIGS. 5 and 6 wherein the voltage along each row increases across the row from left to right, and wherein the duration of the applied voltage pulse along each column increases from top to bottom.

More specifically, voltages V₁, V₂, V₃ . . . V_(m) are applied to columns C₁, C₂, C₃ . . . C_(m), respectively, wherein V₁<V₂<V₃ . . . <V_(m). Also, rows R₁, R₂, R₃ . . . R_(n) are activated for times T₁, T₂, T₃ . . . T_(n), respectively, wherein T₁, <T₂<T₃ . . . <T_(n). To apply a voltage to a given electrode in the first row (Row 1), the TFTs 44 of Row 1 are switched into the conducting state by applying a select signal. The driver voltages in the columns are then set to their predetermined levels and these voltages are passed through the TFTs of Row 1 to the electrodes 34 of the first electrode array within Row 1. During this time, the select signals of the remaining rows are held in the non-select state, so that the remaining electrodes 34 of the first electrode array are connected to their respective row 40 and column 42 conductor via a non-conducting TFT 44 and do not receive a voltage.

After the electrodes 34 in Row 1 are set to the predetermined voltages, the TFTs 44 in Row 1 are again set to the non-conducting state, thereby preventing further change in the voltages of the first row of electrodes.

To apply a voltage to a given electrode 34 in the second row (Row 2), the TFTs 44 in Row 2 are switched into the conducting state by applying a select signal. Again, the driver voltages in the columns are set to their predetermined levels. These may be the same as those applied to Row 1, or different. These voltages are then passed through the TFTs of Row 2 to the electrodes 34 of the first electrode array within Row 2. During this time, the select signals of the remaining rows are held in the non-select state, so that the remaining electrodes 34 of the first electrode array are connected to their respective row 40 and column 42 conductor via a non-conducting TFT 44 and do not receive a voltage.

After the electrodes 34 in Row 2 are set to the predetermined voltages, the TFTs 44 in Row 2 are again set to the non-conducting state, preventing further change in the voltages of the second row of electrodes.

All subsequent rows of electrodes 34 are addressed in similar manner. At the end of this first time frame, all electrodes 34 of the first electrode array have a predetermined voltage applied to them. This voltage will remain on each electrode 34 for the first frame period (typically 1 msec-150 msec). Optionally, a storage capacitor arranged in parallel to the electroporation element can be provided to increase the length of time that the applied voltage remains on each electrode.

In alternative embodiments, the electronic circuit at each volume portion may be modified such that the voltage is held on the electrode even in the case that during the non-addressing period the charge leaks between the electrode and either the common electrode or neighboring electrodes. For example, as illustrated in FIG. 7, the circuit may be modified such that the electrode is connected via a second switch 50 (such as a TFT switch) to a voltage supply line 52. In the case of a TFT switch 50, the first switch 44 is used to set the state of the second switch 50 (either conducting or non-conducting), by applying a voltage to gate of the second switching TFT 50. By storing this voltage on the gate (using either the self capacitance of the second switch, or with a further storage capacitor 54), it is possible to hold the switch in its conducting state for a prolonged period of time. This ensures that the voltage is held on the electrode. Further, to enable more voltage levels, it is possible to connect the electrode to one of a plurality of voltage supply lines using a plurality of further switches.

To realise voltage pulses of different durations, the addressing of different rows in the display may proceed in subsequent time frames.

The voltages applied to the electrode 34 of Row 1 in the first time frame will be present on the electrodes 34 until the following addressing period (in the second time frame) wherein the voltage is set to the same voltage as is present on the common electrode, e.g. 0V. At this point, electroporation stops in row 1. In subsequent time frames, Row 1 is either not addressed (as shown in FIG. 6) or may be repeatedly addressed with a voltage of 0V. However, to apply a voltage of longer duration to the electrodes of Row 2, Row 2 is addressed both in the first time frame and in the second time frame. Alternatively, but less preferably, Row 2 need not be addressed in the second frame, whereby the voltage will be maintained which was applied in the first frame. Thus, the applied voltages are maintained in Row 2 for the second frame. The voltage is then set to 0V only in the third time frame. At this point, electroporation stops in Row 2. It will therefore be appreciated that the duration of the voltages applied to the electrodes 34 of Row 2 is twice that of the electrodes in Row 1.

Similarly, the electrodes 34 of Rows 3, 4 and 5 are applied with progressively larger voltage durations by addressing these rows with the predetermined voltages in further subsequent time frames.

Thus, by using the two axes of the matrix to vary the duration and the amplitude of the electric pulse given to cells positioned in different volume portions, a plurality of cells can be electroporated under different electroporation parameters using a single electroporation procedure. In other words, the electroporation properties of multiple cells may be investigated by generating electric fields of different amplitudes or durations in one or more volume portions of the analysis device.

Once the electroporation procedure is completed, the cells can be inspected or investigated as necessary. Such an investigation process may include the steps of optically inspecting the electroporated cell or measuring parameters of the cells such as their impedance.

FIG. 8 illustrates the operation of the device of FIG. 3 according to another embodiment of the invention. In this embodiment, the matrix is divided into 1 through N one-dimensional arrays of electrodes (A₁ through A_(N)), whereby the voltage along each row of electrodes increases across the row from left to right, and the duration of the applied voltage to each row is substantially the same.

More specifically, voltages V₁, V₂, V₃ . . . V_(m) are applied to columns C₁, C₂, C₃ . . . C_(m), respectively, wherein V₁<V₂<V₃ . . . <V_(m). Also, rows R₁, R₂, R₃ . . . R_(n) are each activated for an equal time TR.

Each array may be sealed to contain cells to be analysed and a different reagent. Thus, using the same matrix, different electroporation experiments may be carried out in parallel, wherein each experiment is undertaken on cells suspended in a particular reagent.

In an alternative, more general embodiment, the device may simply be divided into a multiplicity of sub-arrays, wherein each array contains a different reagent and where the amplitude and the duration of the applied voltage may vary.

From the above description, it will be understood that the embodiment of FIG. 3 has a structure similar to that of a conventional active matrix liquid crystal display (LCD), wherein the liquid crystal has been removed from between the substrates. It is therefore envisaged that known technology and techniques employed to manufacture active matrix LCDs may be used to manufacture a cell analysis device according to an embodiment of the invention.

When compared to that of a passive matrix, the addressing scheme of an active matrix enables the electric charge to be held for a longer time, thereby allowing the electric field to be well established and to remain in a quasi steady state. Furthermore, an active matrix enables fast charging and charge holding which provides fast addressing times and also enables high multiplexing ratios of over 1500. It is also noted that the electrical isolation of each volume portion that is provided in an active matrix device suppresses cross-talk between volume portions, greatly improving accuracy when compared to simple passive matrices.

It should be noted that the above-mentioned embodiments illustrate rather than limit the invention, and that those skilled in the art will be able to design many alternative embodiments without departing from the scope of the claims. The invention may be implemented by means of hardware comprising several distinct elements, and by means of suitably programmed computer. In the device claim enumerating several means, several of these means may be embodied by one and the same item of hardware. 

1. System (10) for providing an improved imaging of an object, the system comprising a plurality of light sources (11, 11 a-11 d) adapted for illuminating the object (12), wherein at least a part of the light sources (11, 11 a-11 d) are adapted to emit light having wavelengths (λ1-λ6) of a different range of wavelengths; a controlling unit (13) adapted for controlling the plurality of light sources (11, 11 a-11 d) so that the plurality of light sources (11, 11 a-11 d) illuminate the object (12) in a subsequent number of illumination periods (T1-T6), wherein in at least two of the subsequent illumination periods (T1-T6) the object (12) is illuminated by wavelengths (λ1-λ6) of a different range of wavelengths; an acquiring unit (14) adapted for acquiring at least four sets of image data (21 a-21 d) of the object (12) in the at least two illumination periods (T1-T6); and a reconstruction unit (15) adapted for reconstructing the at least four acquired sets of image data (21 a-21 d) to a set of image data (22) of an at least four-dimensional colour space.
 2. System of claim 1, further comprising at least four light sources (11 a-11 d) adapted to emit light having wavelengths (λ1-λ6) of a different range of wavelengths.
 3. System of claim 2, wherein the acquiring unit (14) is a monochrome acquisition device.
 4. System of claim 1, wherein the light sources (11, 11 a-11 d) are adapted to emit at least two of the different ranges of wavelengths (λ5, λ6), and wherein at least one of the ranges (λ5, λ6) includes at least two different sub-ranges of wavelengths (λ1, λ3; λ2, λ4); the acquiring (14) unit is adapted to acquire at least two sets of image data (21 a, 21 c; 21 b, 21 d) of the object (12) in each of the at least two illumination periods (T5, T6); and the acquiring unit (15) is sensitive to at least one of the different sub-ranges (λ1, λ3, λ2, λ4) of wavelengths for each of the at least two sets of image data (21 a, 21 c; 21 b, 21 d).
 5. System of claim 1, wherein at least a part of the plurality of light sources (11, 11 a-11 d) are arrange such that the illumination is carried out in a substantially equal angle of incidence for the corresponding wavelengths of the different range of wavelengths.
 6. System of claim 1, wherein the acquiring unit (14) is a multicolour acquisition device.
 7. System of claim 1, wherein the light sources (11, 11 a-11 d) and the acquiring unit (14) are adapted to obtain an reconstructed set of image data (22) of an CIE standard colour space.
 8. System of claim 1, wherein the plurality of light sources (11, 11 a-11 d) cover a wavelength emitting spectrum of substantially 380 nm to 830 nm.
 9. System of claim 1, wherein the light sources (11, 11 a-11 d) comprise one ore more light emitting diodes (18), wherein each of the light emitting diodes (18) are adapted to emit light of a wavelength of one or more different ranges of wavelengths (λ1-λ6).
 10. System of claim 1, wherein the light sources (11, 11 a-11 d) comprise one ore more laser diodes (18), wherein each of the laser diodes (18) are adapted to emit light of a wavelength of one or more different ranges of wavelengths (λ1-λ6).
 11. System of claim 1, wherein the acquisition device is a charged coupled device.
 12. Method for providing an improved imaging of an object, the method comprising illuminating (S1, S3, S5, S7, SO) the object (12) with a plurality of light sources (11, 11 a-11 d) in a subsequent number of illumination periods (T1-T6), wherein at least a part of the light sources (11, 11 a-11 d) emit light having wavelengths of a different range of wavelengths (λ1-λ6), and wherein in at least two of the subsequent illumination periods (T1-T6) the object (12) is illuminated by wavelengths of a different range of wavelengths (λ1-λ6), acquiring (S2, S2 a, S2 b, S4, S8, S8 a, S8 b, SE) at least four sets of image data (21 a-21 d) of the object (12) in the at least two illumination periods (T1-T6), and reconstructing (S10) the at least four acquired sets of image data (21 a-21 d) to an set of image data (22) of an at least four-dimensional colour space.
 13. Method of claim 12, further comprising illuminating (S1, S3, SO) the object (12) in at least four of the subsequent illumination periods (T1-T4) with light sources (11, 11 a-11 d) adapted to emit light having wavelengths of a different range of wavelengths (λ1-λ6) in each of the at least four illumination periods (T1-T4), and acquiring (S2, S4, SE) a set of image data (21 a-21 d) of the object (12) in each of the at least four illumination periods (T1-T4).
 14. Method of claim 12, wherein only one of each light sources (11, 11 a-11 d ) illuminates the object (12) in one of a subsequent number of illumination periods (T1-T4).
 15. Method of claim 13, wherein acquiring (S2, S4, SE) is carried out as a monochrome acquiring.
 16. Method of claim 12, wherein at least two of the different ranges of wavelengths (λ5, λ6) include at least two different sub-ranges of wavelengths (λ1, λ3; λ2, λ4), and the method further comprises acquiring at least two sets of image data (21 a, 21 c; 21 b, 21 d) of the object (12) in each of the at least two illumination periods (T5, T6), wherein the acquiring (S2, S2 a, S2 b, S8, S8 a, S8 b) of each of the at least two sets of image data (21 a, 21 c; 21 b, 21 d) is sensitive to at least one of the different sub-ranges (λ1-λ4) of wavelengths.
 17. Method of claim 16, wherein in each of at least one illumination periods (T5, T6) the at least two sets of image data (21 a, 21 c; 21 b, 21 d) are acquired parallel in time.
 18. Method of claim 12, wherein the illumination periods (T1-T6) of the plurality of light sources (11 a-11 d) are consecutive and/or repeated periodically.
 19. Method of claim 12, wherein the illumination (S1, S3, S5, S7) is carried out in a substantially equal angle of incidence for each of the wavelengths of the different range of wavelengths (λ1-λ4).
 20. Method of claim 12, wherein the acquiring (S1, S3, S5, S7) is carried out as a multicolour acquiring. 21-22. (canceled) 